Newly Identified Lines of Ni xviii, Cu xix, and Zn xx in the Na i Isoelectronic Sequence

Uri Feldman; Leonard Cohen; Marvin Swartz

doi:10.1364/JOSA.57.000535

Journal of the Optical Society of America
Vol. 57,
Issue 4,
pp. 535-536
(1967)
•https://doi.org/10.1364/JOSA.57.000535

Newly Identified Lines of Ni xviii, Cu xix, and Zn xx in the Na i Isoelectronic Sequence

Uri Feldman, Leonard Cohen, and Marvin Swartz

Not Accessible

Your library or personal account may give you access

Get PDF
Email
Share
Get Citation
Copy Citation Text
Uri Feldman, Leonard Cohen, and Marvin Swartz, "Newly Identified Lines of Ni xviii, Cu xix, and Zn xx in the Na i Isoelectronic Sequence," J. Opt. Soc. Am. 57, 535-536 (1967)

Export Citation
- BibTex
- Endnote (RIS)
- HTML
- Plain Text
Citation alert
Save article

Abstract

Lines are reported belonging to Ni xviii, Cu xix, and Zn xx for the following transitions:

3 s {}^{2}S - 4 p {}^{2}P °, 3 p {}^{2}P ° - 4 s {}^{2}S, 3 p {}^{2}P ° - n_{1} d {}^{2}D (n_{1} = 4, 5), and 3 d {}^{2}D - n_{2} f {}^{2}F ° (n_{2} = 4, 5, 6) .

Wavelengths, energies, and term values are given.

Full Article | PDF Article

More Like This

Spectra of Fe, Co, Ni, and Cu Isoelectronic with Na i and Mg i

U. Feldman, L. Katz, W. Behring, and L. Cohen
J. Opt. Soc. Am. 61(1) 91-95 (1971)

New Lines in Isoelectronic Sequences of Argon I from V vi to Ni xi and in Isoelectronic Sequences of Potassium i from Cr vi to Cu xi

E. Alexander, U. Feldman, and B. S. Fraenkel
J. Opt. Soc. Am. 55(6) 650-652 (1965)

Spectra of Ions in the Fluorine i Isoelectronic Sequence from Sc xiii to Cu xxi

Leonard Cohen, U. Feldman, and S. O. Kastner
J. Opt. Soc. Am. 58(3) 331-334 (1968)

Previous Article Next Article

Cited By

You do not have subscription access to this journal. Cited by links are available to subscribers only. You may subscribe either as an Optica member, or as an authorized user of your institution.

Contact your librarian or system administrator
or
Login to access Optica Member Subscription

Tables (3)

You do not have subscription access to this journal. Article tables are available to subscribers only. You may subscribe either as an Optica member, or as an authorized user of your institution.

Contact your librarian or system administrator
or
Login to access Optica Member Subscription

Equations (1)

You do not have subscription access to this journal. Equations are available to subscribers only. You may subscribe either as an Optica member, or as an authorized user of your institution.

Contact your librarian or system administrator
or
Login to access Optica Member Subscription

		Co xvii			Ni xviii			Cu xix			Zn xx
Transition		λ(Å)	Int	ν(cm⁻¹)	λ(Å)	Int	ν(cm⁻¹)	λ(Å)	Int	ν(cm⁻¹)	λ(Å)	Int	ν(cm⁻¹)
3d ²D_5/2–4f	²F_7/2°				52.720^a	8	1 896 800^a	47.437^a	8	2 108 060^a	42.93	8	2 329 400
²D_3/2–	²F_5/2°				52.615^a	7	1 900 600^a	47.329^a	7	2 112 870^a	42.83	7	2 335 100
3p ²P_3/2°–4s	²S_1/2				51.04	3	1 959 200	46.08	3	2 170 100
²P_1/2°–	²S_1/2				50.25	3	1 990 000
3p ²P_3/2°4d	²D_5/2				44.365	7	2 254 000	40.26^b	7	2 483 800	36.74	7	2 721 800
²P_1/2°–	²D_3/2				43.814^a	5	2 282 400^a	39.72	5	2 517 600	36.20	5	2 762 000
3s ²S_1/2–4p	²P_1/2°				41.24	4	2 424 800	37.50	3	2 666 700	34.27	3	2 918 000
²S_1/2–	²P_3/2°				41.03	6	2 437 200	37.30	6	2 681 000	34.08	6	2 934 300
3d ²D_5/2–5f	²F_7/2°	41.462^a	4	2 411 800^a	37.08	4	2 696 900	33.33	4	3 000 300	30.14	3	3 317 900
²D_3/2–	²F_5/2°	41.40	3	2 415 600	37.02	3	2 701 200	33.27	3	3 005 700	30.08	2	3 324 500
3p ²P_3/2°–5d	²D_5/2°	35.92	4	2 784 000	32.34	4	3 092 100	29.29	4	3 414 100	26.62	3	3 756 600
²P_1/2°–	²D_3/2°	35.61	2	2 808 200	32.04	2	3 121 100	29.00	2	3 448 500	26.33	1	3 797 500
3d ²D_5/2–6f	²F_7/2°	35.69	3	2 801 900	31.87	2	3 137 700	28.65	2	3 490 400
²D_3/2–	²F_5/2°

	3s	3d	4s	4d	5d
3p			X	X	X
4p	X
4f		X
5f		X
6f		X

			Co xvii		Ni xviii		Cu xix		Zn xx
Configuration	Designation	J	Level (cm⁻¹)	Interval (cm⁻¹)	Level (cm⁻¹)	Interval (cm⁻¹)	Level (cm⁻¹)	Interval (cm⁻¹)	Level (cm⁻¹)	Interval (cm⁻¹)
3s	3s ²S	$\frac{1}{2}$			0		0		0
3p	3p ²P°	$\frac{1}{2}$			310 600^a		327 700^a		344 700
						30 400		36 100		42 900
		$\frac{3}{2}$			341 000^a		363 800^a		387 600
3d	3d ²D	$\frac{3}{2}$			766 700^a		812 300^a		858 700
						4600		5800		7200
		$\frac{5}{2}$			771 300^a		818 100^a		865 900
4s	4s ²S	$\frac{1}{2}$			2 300 200		2 533 900
4p	4p ²P°	$\frac{1}{2}$			2 424 800		2 666 700		2 918 000
						12 400		14 300		16 300
		$\frac{3}{2}$			2 437 200		2 681 000		2 934 300
4d	4d ²D	$\frac{3}{2}$			2 593 000^b		2 845 300		3 106 700
						2000		2300		2700
		$\frac{5}{2}$			2 595 000		2 847 600		3 109 400
4f	4f ²F°	$\frac{5}{2}$			2 667 400^b		2 925 200^b		3 193 800
						800		1000		1500
		$\frac{7}{2}$			2 668 200^b		2 926 200^b		3 195 300
5d	5d ²D	$\frac{3}{2}$	3 101 800		3 431 700		3 776 200		4 142 200
				1100		1400		1700		2000
		$\frac{5}{2}$	3 102 900		3 433 100		3 777 900		4 144 200
5f	5f ²F°	$\frac{5}{2}$	3 137 100		3 467 900		3 818 000		4 183 200
				100		300		400		600
		$\frac{7}{2}$	3 137 200^b		3 468 200		3 818 400		4 183 800
6f	6f ²F°	$\frac{5}{2}$
		$\frac{7}{2}$	3 527 100		3 909 000		4 308 500
2s²2p^{6 1}S₀	Limit				4 897 400^a		5 410 000^a		5 952 000

		Co xvii			Ni xviii			Cu xix			Zn xx
Transition		λ(Å)	Int	ν(cm⁻¹)	λ(Å)	Int	ν(cm⁻¹)	λ(Å)	Int	ν(cm⁻¹)	λ(Å)	Int	ν(cm⁻¹)
3d ²D_5/2–4f	²F_7/2°				52.720^a	8	1 896 800^a	47.437^a	8	2 108 060^a	42.93	8	2 329 400
²D_3/2–	²F_5/2°				52.615^a	7	1 900 600^a	47.329^a	7	2 112 870^a	42.83	7	2 335 100
3p ²P_3/2°–4s	²S_1/2				51.04	3	1 959 200	46.08	3	2 170 100
²P_1/2°–	²S_1/2				50.25	3	1 990 000
3p ²P_3/2°4d	²D_5/2				44.365	7	2 254 000	40.26^b	7	2 483 800	36.74	7	2 721 800
²P_1/2°–	²D_3/2				43.814^a	5	2 282 400^a	39.72	5	2 517 600	36.20	5	2 762 000
3s ²S_1/2–4p	²P_1/2°				41.24	4	2 424 800	37.50	3	2 666 700	34.27	3	2 918 000
²S_1/2–	²P_3/2°				41.03	6	2 437 200	37.30	6	2 681 000	34.08	6	2 934 300
3d ²D_5/2–5f	²F_7/2°	41.462^a	4	2 411 800^a	37.08	4	2 696 900	33.33	4	3 000 300	30.14	3	3 317 900
²D_3/2–	²F_5/2°	41.40	3	2 415 600	37.02	3	2 701 200	33.27	3	3 005 700	30.08	2	3 324 500
3p ²P_3/2°–5d	²D_5/2°	35.92	4	2 784 000	32.34	4	3 092 100	29.29	4	3 414 100	26.62	3	3 756 600
²P_1/2°–	²D_3/2°	35.61	2	2 808 200	32.04	2	3 121 100	29.00	2	3 448 500	26.33	1	3 797 500
3d ²D_5/2–6f	²F_7/2°	35.69	3	2 801 900	31.87	2	3 137 700	28.65	2	3 490 400
²D_3/2–	²F_5/2°

	3s	3d	4s	4d	5d
3p			X	X	X
4p	X
4f		X
5f		X
6f		X

Abstract

Cited By

Tables (3)

Equations (1)

Journal of the Optical Society of America